WO2009054715A1

WO2009054715A1 - Multlmode fiber

Info

Publication number: WO2009054715A1
Application number: PCT/NL2008/000239
Authority: WO
Inventors: Denis Molin; Yves Lumineau; Pierre Sillard; Ralph Petrus Johannes Adrianus Van Lankveld; Koen De Jongh
Original assignee: Draka Comteq B.V.
Priority date: 2007-10-23
Filing date: 2008-10-23
Publication date: 2009-04-30
Also published as: US8724950B2; KR20100075945A; US20110305423A1; CN101836144A; US8009950B2; KR101554373B1; EP2203767A1; FR2922657A1; DK2203767T3; EP2203767B1; US20100254653A1; WO2009054715A8; FR2922657B1

Abstract

A multimode optical fiber comprises a central core having an alpha profile, a depressed cladding having a portion in continuity with the alpha profile of the central core and a stepped portion, and an outer cladding. The alpha profile is obtained by co-doping at least two dopants. The variation in concentration of each dopant and its derivative in relation to the fiber radius are continuous. A multimode fiber for Ethernet optical system with an improved bandwidth is thus obtained.

Description

MULTIMODE FIBER

The present invention concerns the field of optical fiber transmissions, and more specifically a multimode optical fiber. The multimode optical fibers are particularly used for short-distance transmission systems requiring a large bandwidth.

An optical fiber conventionally consists of an optical core, whose function is to transmit and possibly to amplify an optical signal, and of an optical cladding whose function is to confine the optical signal within the core. For this purpose, the refractive indexes of the core n_c and of the outer cladding n_g are such that n_c>n_g.

For short-distance applications and for local networks, multimode fibers are frequently used. The core of a multimode fiber generally has a diameter of approximately 50 μm, compared with approximately 9 μm for the core of a single mode fiber. Therefore, for a given wavelength, several optical modes propagate simultaneously along the fiber, conveying the same information. The bandwidth is directly related to the group velocity of the optical modes propagating in the multimode core of the fiber. To guarantee a large bandwidth, the group velocities of all the modes must be identical, i.e. the intermodal dispersion must be zero or at least minimized for a given wavelength. Multimode fibers have been the subject of international standardization under standard ITU-T G.651 (withdrawn on August 16, 2008) and the improved standard ITU-T G.651.1 (approved on July 29, 2007) which in particular defines criteria for modal bandwidth-length product for overfilled launch [minimum at 850 nm of 500 Mhz.km and minimum at 1300 nm of 500 Mhz.km], numerical aperture [0.20 ± 0.015] and core diameter [50 ± 3 μm], required for compatibility between fibers. The recommended multimode fibre supports the cost- effective use of 1 Gbit/s Ethernet systems over link lengths up to 550 m, usually based upon the use of 850 nm transceivers.

For optical fibers, the refractive index profile is generally presented as a graph plotting the refractive index against the fiber radius. Conventionally the distance r to the center of the fiber is shown along the abscissa, and the difference between the refractive index and the refractive index of the fiber cladding is shown along the ordinate axis. The refractive index profile is therefore referred to as a "step", "trapezoidal", "triangular" or "alpha" profile for graphs having the respective shapes of a step, trapezoid, triangle or gradient. These curves are generally representative of the theoretical or set profile of the fiber, the manufacturing stresses of the fiber possibly leading to a slightly different profile.

In step index fibers, having a "step" core profile, the different modes propagate at different speeds along the fiber, which causes spreading of the light pulse which may become comparable to the spacing between pulses, and lead to an unacceptable error rate. To reduce intermodal dispersion in a multimode fiber, it has been proposed to manufacture graded-index fibers with an "alpha" core profile. Such fibers have been used for many years and its characteristics have been described in particular in the publications: "Multimode theory of graded-core fibres" by D. Gloge et a/., Bell System Technical Journal 1973 pp 1563-1578, and "Comprehensive theory of dispersion in graded-index optical fibers" by G. Yabre, Journal of Lightwave Technology, February 2000, vol. 18, n° 2, pp 166-177.

A graded-index or alpha profile can be defined as the relation between the value n of the refractive index at one point in relation to the distance r from this point to the center of the fiber:

where α > 1 ; (α → _∞ corresponding to a step index); n,, the maximum refractive index value of the multimode core; a, the radius of the multimode core; and

where n₀ is the minimum refractive index value of the multimode core, generally corresponding to the refractive index value of the cladding (which is most often of silica).

A graded-index multimode fiber therefore has a core profile with radial symmetry such that, along any radial direction, the value of the refractive index decreases continuously from the center of the fiber towards its periphery. When a multimode light signal propagates in said graded-index core, the different modes see a different propagation medium, which has a different effect on their speed of propagation. By adjusting the value of parameter α, it is therefore possible to obtain a group speed that is practically equal for all the modes and hence a reduced intermodal dispersion.

This adjustment of parameter α theoretically allows a group speed to be obtained that is practically equal for all the modes, but the profile of the multimode fiber actually manufactured comprises a graded-index central core surrounded by an outer cladding with constant refractive index. Therefore the core of the multimode fiber never corresponds to a perfect alpha profile since the interface with the outer cladding interrupts this alpha profile. Modes of highest order will therefore be accelerated relative to the lower order modes, and the bandwidth will necessarily thereby be reduced. This phenomenon, known under the expression "cladding effect" is seen when measuring modal dispersion delay, which shows multiple response pulses when the majority of excited modes are the highest order modes.

This problem has already been identified. To solve this problem, it has been proposed to insert an intermediate depressed cladding between the graded-index core and the outer cladding. The alpha profile of the core is therefore extended into a depressed cladding. Said solution is described in particular in document WO-A-2006/010798 in which the core is formed by controlled Germanium doping (up dopant) and the depressed cladding is obtained by doping with Fluorine (down dopant).

Such a solution requires perfect control over the dopant concentrations to guarantee continuity of the alpha profile, in particular at the core/depressed cladding boundary. In practice, it is almost impossible to ensure continuity of the slopes, i.e. a smooth slope profile without sudden changes in the slope of refractive index profiles of the core (doped with Germanium) and of the depressed cladding (doped with Fluorine). This rupture or discontinuity of slope in the alpha profile caused by a switch of an up dopant for a down dopant causes pertubations for transmission of the highest order modes, and consequently a reduction in the bandwidth. Document US-A-4 339 174 describes a multimode fiber with a core having a graded-index profile and a rupture point. Such a rupture point can cause pertubations however in fast bit rate transmissions.

Documents US-A-4 229 070 and US-A-4 230 396 describe multimode fibers having profiles obtained by co-doping in the core and in the depressed cladding surrounding the core.

For applications of fast bit rate Ethernet networks over long-haul distances, in particular for bit rates of 10 GbE (10 Gb/s) or higher, over more than 300 m (respectively 550m), the guaranteed effective bandwidth must be 2000 MHz-km or greater (respectively 4700 MHz-km). Standard TIA-492AAAC-A standardizes the performance levels required for fast rate multimode fibers of diameter 50 μm. For multimode fibers, the bandwidth depends on the source used. The effective bandwidth (called EMB for Effective Modal Bandwidth) corresponds to the smallest bandwidth for all the EMBs of Source-Fiber pairs for all standardized sources in 10 GbE applications. In order to attain the performance levels laid down by standards, it is necessary to eliminate any discontinuity or rupture of the slope of the alpha profile which could occur at the interface between the core and the depressed cladding.

There is therefore a need for a multimode fiber which has a graded-index core with an alpha profile which extends into a depressed cladding without any slope rupture in the profile.

For this purpose, the invention proposes fabricating the total alpha profile by co-doping with at least two dopants. One dopant increasing the refractive index of silica, e.g. Germanium, is predominant in the core and one dopant reducing the refractive index of silica e.g. Fluorine, is predominant in the depressed cladding. However, both dopant are present in both the core and the depressed cladding. The concentration of each dopant is controlled so as to obtain a continuous variation and a continuous derivative with respect to the fiber radius. In the present invention, the expression "continuous variation" is used opposite to discrete variation i.e. the concentrations of each dopant are controlled so as to avoid any perceptible shift in value. This continuity of variation and slope ensures continuity of the alpha profile and limits modal dispersion in the multimode fiber. Hence not only the concentration itself should increase or decrease in a continuous manner but also the first derivative of the concentration relative to the radius should increase or decrease in a continuous manner.

The invention therefore concerns a multimode optical fiber comprising: - a central core having an alpha profile; a depressed cladding having a portion in continuity with the alpha profile of the central core and a stepped portion; an outer cladding; wherein the alpha profile and the portion in continuity with the alpha profile of the depressed cladding are obtained by co-doping with at least two dopants, the variation in the concentration of each dopant and its derivative in relation to the fiber radius being continuous.

It should be noted that the phrase "alpha profile" relates to the central core having a "alpha" shape and having a refractive index higher than the refractive index of the outer cladding. The phrase "a portion in continuity with the alpha profile" is that portion of the depressed cladding having an "alpha" shape and having a refractive index lower than the refractive index of the outer cladding.

According to one embodiment, at least one dopant of the alpha profile is a dopant increasing the refractive index of silica, the concentration of said dopant being zero in the stepped portion of the depressed cladding.

According to one embodiment, the stepped portion of the depressed cladding has a width of 2 μm or less; this stepped portion of the depressed cladding may have a refractive index difference with the outer cladding equal to or greater than 5.10^"3, meaning that the refractive index is equal to -5.10^"3 or lower being deeper buried.

According to one embodiment, the dopants of the alpha profile and the portion in continuity with the alpha profile comprise Germanium and Fluorine.

According to one application, the fiber has a central core diameter of 50 μm and a numerical aperture of 0.2 ± 0.015. Other characteristics and advantages of the invention will become apparent on reading the following description of embodiments of the invention given as examples and with reference to the appended drawings which show: figure 1 , a graphical illustration of the set refractive index profile of a multimode fiber of the invention; figure 2, a graphical illustration of concentrations of Germanium and Fluorine in a multimode fiber of the prior art; figure 3, a graphical illustration of the concentration of Germanium and Fluorine in a multimode fiber of the invention; - figure 4, a graph illustrating the difference between the refractive index profiles of a prior art fiber and a fiber according to the invention respectively with an ideal alpha profile.

The fiber of the invention is a multimode transmission fiber. It has a refractive index profile such as illustrated in figure 1. It has a central core having a graded-index (alpha) profile which extends into a depressed cladding. The core, has a standardized radius of 25 μm. Within the context of the present invention, by "central core" of the fiber is meant a region in which most of the energy of the optical signal is confined, i.e. the region for which the refractive index n is greater than the refractive index of the outer cladding n>n_g. The outer cladding is typically of natural silica for cost related reasons, but could also be of doped silica.

The depressed cladding therefore has a portion in continuity with the alpha profile of the core, and a stepped portion having a constant refractive index lower than the refractive index of the outer cladding. By depressed cladding is meant the radial portion of the fiber whose refractive index value is lower than the refractive index of the outer cladding n_g.

The fiber of the invention therefore has a core with an alpha profile, but this alpha profile goes beyond the core stricto sensu since it extends into the depressed cladding. The value of the alpha coefficient of the graded-index profile is adjusted according to the application for which the multimode fiber is intended. In the profile shown in figure 1 , alpha lies between 2.1 and 2 at a wavelength of 633 nm. As is well known to persons skilled in the art, the theoretical alpha profile is difficult to reproduce on actual profiles of manufactured optical fibers. No depositing method is sufficiently precise for the actual profile of the fabricated fiber to have the form of the theoretical alpha profile, and no profile measurement apparatus currently has the required accuracy to give an exact alpha value. Reference can be made to the publication by P. Matthijsse et al "On the Design of Wide Bandwidth Window Multimode Fibers" for the determination of an optimal alpha value in relation to wavelength. The fiber of the invention is compatible with standard G.651 and G.651.1. It has a core diameter of 50 μm, a numerical aperture of 0.2 ± 0.015, and bandwidth greater than 2000 MHz-km (respectively 4700 MHz-km) with a modal dispersion of less than 0.3 ps/m (respectively 0.14 ps/m). The profile in figure 1 could be obtained with the doping concentrations illustrated in figure 2 which is not part of the invention. In figure 2, the central core is obtained by controlled doping with Germanium, the concentration of Germanium (thick black line) becoming zero at the interface with the depressed cladding. The depressed cladding is obtained by controlled doping with Fluorine (thin grey line) the concentration of Fluorine being zero in the core.

As set forth above, such a change of dopant at the core/depressed cladding is difficult to control and cannot guarantee continuity of the alpha profile, which causes perturbations in the transmission of the signal and reduces the size of the bandwidth which can be used in the multimode fiber. The invention therefore proposes, as illustrated in figure 3, to conduct co-doping of all the alpha profile. The central core therefore contains Germanium (thick black line) and Fluorine (thin grey line) in controlled concentrations to reach the set profile, and the portion of depressed cladding extending the alpha profile also contains Germanium and Fluorine. On the other hand, the stepped portion of the depressed cladding, surrounding the alpha profile, does not contain any Germanium. The stepped portion of the depressed cladding is therefore only doped with Fluorine, which limits fabrication costs of the fiber. The stepped portion of the depressed cladding has a constant refractive index difference with the outer cladding that is equal to or greater than 5.10^"3, meaning that the index is equal to - 5.10^"3 or lower being deeper buried for proper limiting of the cladding effect on the highest order modes. This stepped portion of the depressed cladding is also relatively narrow, its width being 2 μm or less, to allow the portion in continuity with the alpha profile to be as large as possible without modifying the outer diameter of the fiber which is standardized. The fiber of the invention can be manufactured by drawing from a preform using a PCVD technique (Plasma Chemical Vapor Deposition) which allows good incorporation of the Fluorine in the silica. As no Germanium is present in the stepped portion of the depressed cladding, this limits the quantity of Fluorine to be incorporated and reduces manufacturing costs. It can be seen in figure 3 that, on all the alpha profile, the variation in concentration of each dopant and the derivative of this variation are continuous. Any discontinuity in the slope of the alpha profile can therefore be avoided at the interface between the core and the depressed cladding, and any discontinuity in the alpha profile is thereby limited.

A profile that is closer to the ideal alpha profile can therefore be achieved. Figure 4 illustrates the difference between the theoretical profile and the refractive index profiles of a multimode fiber without co-doping (thin grey line) and a multimode fiber of the invention with co-doping (thick black line) respectively. It will be noticed that the profile of the fiber of the invention is closer to the ideal profile, and in particular that discontinuity at the core/depressed cladding interface is eliminated.

The multimode fiber of the invention can be used in an Ethernet optical system with an improved bandwidth. It should be noted that the present invention is not limited to the embodiments described as examples. In particular, dopants other than Germanium and Fluorine can be used, provided the set profile is observed and provided the variation and variation derivative of the dopant concentrations are continuous.

Claims

1. A multimode optical fiber, comprising from the center to the periphery: - a central core having an alpha profile;

- a depressed cladding having a portion in continuity with the alpha profile of the central core and a stepped portion;

- an outer cladding; wherein the alpha profile and the portion in continuity with the alpha profile are obtained by co-doping with at least two dopants, the variation in concentration of each dopant and its derivative in relation to the fiber radius being continuous with respect to the fiber radius.

2. The fiber of claim 1 , wherein at least one dopant of the alpha profile is a dopant increasing the refractive index of silica, the concentration of said dopant being zero in the stepped portion of the depressed cladding.

3. The fiber of claim 1 or 2, wherein the stepped portion of the depressed cladding has a width being inferior or equal to 2 μm.

4. The fiber of any one of claims 1 to 3, wherein the stepped portion of the depressed cladding has a refractive index difference with the outer cladding being equal than or lower than -5.10^'3.

5. The fiber of any one of claims 1 to 4, wherein the co-dopants of the alpha profile comprise Germanium and Fluorine.

6. The fiber of any one of claims 1 to 5, wherein the central core has a diameter of 50 μm.

7. The fiber of any one of claims 1 to 6, having a numerical aperture of

0.2 ± 0.015.